Using long-range transmissions in the Beaufort Gyre to test the sound-speed equation at high pressure and low temperature

Author:

Vazquez Heriberto J.1ORCID,Cornuelle Bruce D.1,Worcester Peter F.1ORCID,Dzieciuch Matthew A.1ORCID,Colosi John A.2ORCID,Nash Jonathan D.3

Affiliation:

1. Scripps Institution of Oceanography, University of California San Diego 1 , La Jolla, California 92093, USA

2. Department of Oceanography, Naval Postgraduate School 2 , Monterey, California 93943, USA

3. College of Earth, Atmospheric, and Ocean Sciences, Oregon State University 3 , Corvallis, Oregon 97331, USA

Abstract

An ocean acoustic tomography array with a radius of 150 km was deployed in the central Beaufort Gyre during 2016–2017 for the Canada Basin Acoustic Propagation Experiment. Five 250-Hz transceivers were deployed in a pentagon, with a sixth transceiver at the center. A long vertical receiving array was located northwest of the central mooring. Travel-time anomalies for refracted-surface-reflected acoustic ray paths were calculated relative to travel times computed for a range-dependent sound-speed field from in situ temperature and salinity observations. Travel-time inversions for the three-dimensional sound-speed field consistent with the uncertainties in travel time [∼2 ms root mean square (rms)], receiver and source positions (∼ 3 m rms), and sound speed calculated from conductivity-temperature-depth casts could not be obtained without introducing a deep sound-speed bias (below 1000 m). Because of the precise nature of the travel-time observations with low mesoscale and internal wave variability, the conclusion is that the internationally accepted sound-speed equation (TEOS-10) gives values at high pressure (greater than 1000 m) and low temperature (less than 0 °C) that are too high by 0.14–0.16 m s−1.

Funder

Office of Naval Research

Publisher

Acoustical Society of America (ASA)

Subject

Acoustics and Ultrasonics,Arts and Humanities (miscellaneous)

Reference33 articles.

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2. Linearized travel time, intensity, and waveform inversions in the ocean sound channel—A comparison;J. Acoust. Soc. Am.,1984

3. The Arctic Ocean warms from below;Geophys. Res. Lett.,2012

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